https://doi.org/10.1351/goldbook.P04952
Transient absorption @S05848@ using two pulses (strong pump and weak probe) and capable of achieving a high temporal resolution. A pump pulse excites the sample and triggers the process under investigation. A second delayed pulse, the probe, monitors an optical property. By varying the time delay between the pump and probe pulses, it is possible to assemble measurements as a function of time. The probe pulse is typically a UV, @VT07496@ or @IT07399@ pulse in which case a snap-shot spectrum is taken as a function of the delay time. Often the probe pulse is generated from a portion of the excitation beam, but it can also be an independently generated electromagnetic pulse.
Note:
In the case of an optical probe, this interaction is formally a non-linear optical process that is third-order in @P04712@. The excitation intensity to create the @E02257@ constitutes a two-field interaction and the determination of the change in the time-dependent optical properties involves a third field @MT06831@ the induced time-dependent changes in the 'linear susceptibility'. Diffractive probes (e.g., electrons and X-rays) can also be used, in which case one measures a @D01711@ pattern as a function of time.
In the case of an optical probe, this interaction is formally a non-linear optical process that is third-order in @P04712@. The excitation intensity to create the @E02257@ constitutes a two-field interaction and the determination of the change in the time-dependent optical properties involves a third field @MT06831@ the induced time-dependent changes in the 'linear susceptibility'. Diffractive probes (e.g., electrons and X-rays) can also be used, in which case one measures a @D01711@ pattern as a function of time.